Checking Physics Homework: Spring-Tray-Particle System

[Chileboy]

Hi fellow physicists, I have some homework problems I'm trying to work through and i need to know if I'm on the right track.

This is the problem:

A Spring is upright (vertical) and has a constant k and a length Lo, a tray of M mass is attached to the spring and on the tray is placed a particle of m mass, suppose you initially compress the spring a distance d from the equilibrium point of the spring-tray-particle system. Calculate the maximum height above the ground the particle will reach.

First i calculated the equilibrium point of the spring-tray-particle system:

(Lo-L1)k = (M+m)g => L1 = Lo - (M+m)g/k

Then I used the conservation of energy, Potencial energy when the spring is compressed = to kinetic energy at equilibrium point.

k(d^2)/2=(M+m)(v^2)/2 => v=sqrt(k/(M+m))d

Then i used the velocity to calculate the height above L1

h= k(d^2)/2g(M+m)

So the height above the ground is

L1 + h = Lo + (M+m)g/k +k(d^2)/2g(M+m)

Is this right? i'd appreciate it if some one could double check it for me.

Thanks in advance. By the way how do you use the special font for numbers and mathematical symbols?

 

[arildno]

Good try! (and great that you provided your calculations)
However, it is incorrect to assume that the particle will leave the tray when the system is at the equilibrium point of the system!

I'll break this into a few steps:
1. Condition of leaving plate:
Normal force N acting on particle is zero (agreed?)
In particular, regarding Newton's second law for the particle, what does this mean that the acceleration of the particle must be then?
2. System of tray+particle
At the point when the particle is about to leave the tray, this system has the acceleration from 1.); what does this imply about the length of the spring?
3. Proceed to find the initial velocity as you've done; your approach here looks fine.

 

[Chileboy]

Lets see.. N=0 when a =0 is that right? does that mean the particle will come off the tray at Lo?

 

[Chileboy]

Okay another problem...

A ring (mass = M) is suspended by an ideal cord from the ceiling, two equal masses (mass = m) are released from the top of the ring and slide down, one on either side of the ring, without friction. The question is:
What condition must the masses meet in order for the ring to move up?

I'm having trouble imagining it, I can't see which force could make the ring go up, possibly the normal of the sliding masses but i don't know how to balance the ecuations.

I hope it doesn't look like I am trying to get someone else to do my homework, i just need some help getting started. Thanks in advance for any help.

 

[arildno]

Lets see.. N=0 when a =0 is that right? does that mean the particle will come off the tray at Lo?

Newton's 2.law for the particle reads:
N-mg=ma
That is, N=0 implies a=-g

 

[Chileboy]

Okay i hope I've got this right, does that mean that the particle will come off the tray at Lo + (M+m)g/k i.e when the force applied by the spring is equal to -(M+m)g?

 

[arildno]

Mm..no!
I didn't say your suggestion of L0 was wrong (it is in fact right!)
Reason:
Let's look at the system tray+particle.
Up to the point of separation, they move and accelerate as a single object.
Newton's 2.law reads:
-k(L(t)-L_{0})-(M+m)g=(M+m)a
Hence, when a=-g, L(t)=L_{0}

 

[Chileboy]

Right i forgot to put -(M+m)g in the force equation, thanks for the help.
I wonder if you could help me with the second problem i posted i cant't really get my head around it. P.S. How do you use the special font for numbers and mathematical symbols?

 

[arildno]

Just click on the line to see how the LATEX code is generated.
(Was that the second problem?)

 

[Chileboy]

The second problem is a bit futher up in this thread.

 

[arildno]

All right, I'll have a look at it..

 

[arildno]

OK, now I've thought about it:
1. You're right about the forces which may push the circle upwards.
If the normal force acting upon a particle from the circle provides a part of the necessary centripetal acceleration of the particle (that is, the particle's gravity is not enough), then the particles will exert an upwards directed force on the circle if they are on the upper half of the circle.

2. If the circle is to be lifted, a necessary condition is that at some time, the tension in the cord becomes 0.
Prior to this moment, the circle will remain at rest.
This will give us one equation.
3. The two particles' path are, of course, symmetric about the vertical axis.
4. Up to the point where the circle might start to move upwards, a given particle's mechanical energy must remain constant.
This provides us with a relation between the angle displacement of the particle (measured with respect to the vertical) and its (angular) velocity about the circle.
5. Now, consider the radial component of a particle's Newton's 2.law:
Clearly, we must require in order for a raising of the circle, that the expressions gained from the equations found in 2. and 4., is consistent with that Newton's 2.law for that particle must have a solution!
This will give you a desired relation between M and m.
I'd like you to try this out by yourself first; I got M\leq\frac{2}{3}m
If you found any of this unclear; just post a reply, I'll get back with the maths later on.

 

[Chileboy]

That's the right answer, i'll try my best to work it out tonight.
I'd appretiate you posting your workings though!

 

[Chileboy]

Let's see.. the centripedal acceleration has to be v^2/r of which cos(alpha)g is given by gravity, so N =m(v^2/r -cos(alpha)g) perpendicular to the circle and cos(alpha)N is the force that could lift the circle. From conservation of energy for the particles i get v^2= 2rg(1-cos(alpha)). N=m(2g-3gcos(alpha)). Is that right so far...

 

[arildno]

What you've written seems almost right, I'll post my own:
1. Normal forces acting on the circle
Clearly, we may write the normal forces from the particles as:
N(\pm\sin\theta\vec{i}+\cos\theta\vec{j}),
where N is the magnitude, and the sign in the horizontal component signifies which particle produce the force.
Hence, net normal force on the circle is:
\vec{N}_{net}=2N\cos\theta\vec{j}
2. The cord tension must be zero:
For the circle at rest, the vertical component of Newton's 2.law reads:
T+2N\cos\theta-Mg=0
or, when T=0,
N=\frac{Mg}{2\cos\theta}
3. Conservation of a particle's mechanical energy:
This is simply, while the circle is at rest:
\frac{1}{2}m\vec{v}^{2}+mgR\cos\theta=mgR
where the reference level for potential energy has been chosen at \theta=\frac{\pi}{2}
Or:
\frac{m\vec{v}^{2}}{R}=2mg(1-\cos\theta)

4.Radial component of Newton's 2.law for the particle:
This is, in general:
-N-mg\cos\theta=-m\frac{\vec{v}^{2}}{R}
Inserting relations from 2+3, and eliminating "g":
\frac{M}{2\cos\theta}=2m-3m\cos\theta

Rearranging, we have:
3m\cos^{2}\theta-2m\cos\theta+\frac{M}{2}=0
Or:
\cos\theta=\frac{1}{3}(1\pm\sqrt{1-\frac{3M}{2m}})
Clearly, we must require real solutions, so:
M\leq\frac{2}{3}m

 

[Chileboy]

I actually got the result on my own in the end which is very satisfying. Thanks for taking so much time to help me out.

 

[arildno]

Great that you managed it on your own!